| Lines 1-4 were replaced by lines 1-4 |
| - !Pressure devices are available in cooperation with the responsible members of LNS.\\ |
| - !Before writing a proposal involving pressure, please check the feasibility both with the instrument scientist, and the relevant person responsible for the pressure cell:\\ |
| - *[J. White|https://www.psi.ch/lns/jonathan-white]: clamp cells - single crystal inelastic and elastic neutron scattering, Paris-Edinburgh Press - powder samples, single crystals in optimal circumstances.\\ |
| - *[D. Sheptiakov|https://www.psi.ch/lns/denis-cheptiakov]: clamp cells - powder neutron diffraction.\\ |
| + !Neutron pressure devices are available in cooperation with the responsible members of LNS.\\ |
| + !Before writing a proposal involving pressure, please check the feasibility with ''both'' the instrument scientist, and the relevant pressure cell responsible:\\ |
| + *[J. White|https://www.psi.ch/lns/jonathan-white]: clamp cells - single crystal inelastic and elastic ns, Paris-Edinburgh Press - powder elastic ns, single crystal elastic ns in favourable cases.\\ |
| + *[D. Sheptiakov|https://www.psi.ch/lns/denis-cheptiakov]: clamp cells - powder elastic ns.\\ |
| Lines 6-12 were replaced by lines 6-7 |
| - ||Name||Description||Range||Used in||Dim |
| - |[P9] |clamp cell for elastic ns | <9 kbar|ILL2, ILL5|d=7, c=20 |
| - |[P15]|clamp cell for elastic ns |<15 kbar|ILL2, ILL5|d=7, c=20 |
| - |[P10]|clamp cell for inelastic ns|<10 kbar|ILL2, ILL5|d=7, c=20 |
| - |[P18]|clamp cell for inelastic ns|<18 kbar|ILL5 |d=7, c=20 |
| - |[P30]|single crystal clamp cell for elastic ns|<30 kbar|APD |d=4, c=8 |
| - |[PE] |Paris-Edinburgh press (opposed anvils)|<100 kbar|RT |d=5, c=1.5 |
| + Below is a link to a file that provides an overview of the routinely available pressure options at SINQ.\\ |
| + [Summary of Pressure Cell Options at SINQ (updated Oct' 2016)|Pcells_at_SINQ_PSI_Oct_2016.pdf] |
| At line 13 added 9 lines. |
| + Crucial information concerning each routinely available pressure device is summarised in the table below.\\ |
| + ||Name||Contact||Description||Range||Used in||Suitable Beamlines||Dim |
| + |[P10]|JW|clamp cell for single crystal inelastic or elastic ns|10-12 kbar at RT, 8-10 kbar at 1.5K|ILL2, ILL5|FOCUS, TASP, RITA-II, EIGER, ZEBRA|d=7, c=25 |
| + |[P17]|JW|clamp cell for single crystal inelastic or elastic ns|15-17 kbar at RT, 13-15 kbar at 1.5K|ILL5|FOCUS, TASP, RITA-II, EIGER, ZEBRA|d=7, c=25 |
| + |[P15]|DS|clamp cell for powder elastic ns|13-15 kbar at RT, 12-14 kbar at 1.5K|ORI4,ILL5|HRPT, DMC|d=8, c=25 |
| + |[P10_NMS]|JW|non-magnetic clamp cell for single crystal inelastic or elastic ns|8-10 kbar at RT, 7-8 kbar at 1.5K|ILL2, ILL5, MA09, MA07|FOCUS, TASP, RITA-II, EIGER, ZEBRA, SANS-I, SANS-II|d=8, c=20 |
| + |[P10_NMP]|DS|non-magnetic clamp cell for powder elastic ns|8-10 kbar at RT, 7-8 kbar at 1.5K|ORI4, MA09, MA07|HRPT, DMC|d=6, c=25 |
| + |[PE]|JW|Paris-Edinburgh press (opposed anvils)|100 kbar at RT, 50kbar at 20K|The press has a RT mode, or a dedicated CCR for low T mode|HRPT, DMC for powders, RITA-II for single crystal|d=5, c=1.5 |
| + |
| Line 16 was replaced by lines 20-39 |
| - c: useable sample height |
| + c: useable sample height\\ |
| + |
| + Recent SINQ publications using high pressure (these can give you an idea of what can be achieved at SINQ):\\ |
| + *Dimensional reduction by pressure in the magnetic framework material CuF2(D2O)2(pyz): From spin-wave to spinon excitations, [Phys. Rev. B 96,020414(R) (2017)|https://journals.aps.org/prb/abstract/10.1103/PhysRevB.96.020414] |
| + *Stress-induced magnetic domain selection reveals a conical groundstate for the multiferroic phase of Mn2GeO4, [Phys. Rev. B 94,024439 (2016)|http://journals.aps.org/prb/abstract/10.1103/PhysRevB.94.024439] |
| + *Pressure-induced spin reorientation and spin state transition in SrCoO3, [Phys. Rev. B 92,195147 (2015)|http://journals.aps.org/prb/abstract/10.1103/PhysRevB.92.195147] |
| + *Pressure dependence of the magnetic order in CrAs: a neutron diffraction investigation, [Phys. Rev. B 91,020409(R) (2015)|http://journals.aps.org/prb/abstract/10.1103/PhysRevB.91.020409] |
| + *High pressure induced spin state crossover in Sr2CaYCo4O10.5, [J. Phys.: Condens. Matter 27, 046005 (2015)|http://iopscience.iop.org/article/10.1088/0953-8984/27/4/046005/meta] |
| + *Equation-of-state of lead from high-pressure neutron diffraction up to 8.9 GPa and its implication for the NaCl pressure scale, [Phys. Rev. B 90, 014101 (2014)|http://journals.aps.org/prb/abstract/10.1103/PhysRevB.90.014101] |
| + *Pressure effect on magnetism and multiferroicity in Mn2GeO4, [Phys. Rev. B 89, 104405 (2014)|http://journals.aps.org/prb/abstract/10.1103/PhysRevB.89.104405] |
| + *Magnetic ordering in Fe1.087Te under pressure, [European Physical Journal B 86, 18 (2013)|http://link.springer.com/article/10.1140%2Fepjb%2Fe2012-30528-9] |
| + *Coexistence of superconductivity and magnetism in FeSe1−x under pressure, [Phys. Rev. B 85, 064517 (2012)|http://journals.aps.org/prb/abstract/10.1103/PhysRevB.85.064517] |
| + *Elastic properties of alpha-iron at high temperatures by high-pressure neutron scattering, [Journal of Physics D - Applied Physics 44, 055406 (2011)|http://iopscience.iop.org/article/10.1088/0022-3727/44/5/055406/meta] |
| + *Competition between ferromagnetic and antiferromagnetic ground states in multiferroic BiMnO3 at high pressures, [Phys. Rev. B 82, 014401 (2010)|http://journals.aps.org/prb/abstract/10.1103/PhysRevB.82.014401] |
| + *Pressure effects on the magnetic structure in La0.5Ca0.5-xSrxMnO3 (0.1 < x < 0.4) manganites, [Phys. Rev. B 81, 104424 (2010)|http://journals.aps.org/prb/abstract/10.1103/PhysRevB.81.104424] |
| + *Study of diffuse scattering under hydrostatic pressure in PbMg1/3Nb2/3O3, [J. Phys. Conf. Series 251, 012011 (2010)|http://iopscience.iop.org/article/10.1088/1742-6596/251/1/012011/meta] |
| + *Temperature dependence of the pressure-induced amorphization of ice I-h studied by high-pressure neutron diffraction to 30 K, [Phys. Rev. B 82, 094103 (2010)|http://journals.aps.org/prb/abstract/10.1103/PhysRevB.82.094103] |
| + *Atomic displacements in PbMg1/3Nb2/3O3 under high pressures, [J. Phys.: Condens. Matter 20, 104235 (2008)|http://iopscience.iop.org/article/10.1088/0953-8984/20/10/104235] |
| + *The alpha-gamma-epsilon triple point of iron investigated by high pressure-high temperature neutron scattering, [App. Phys. Lett. 93, 091904 (2008)|http://scitation.aip.org/content/aip/journal/apl/93/9/10.1063/1.2976128] |
| + *High-pressure behavior of CsC8 graphite intercalation compound: Lattice structures and phase-transition mechanism, [Phys. Rev. B 77, 125433 (2008)|http://journals.aps.org/prb/abstract/10.1103/PhysRevB.77.125433] |
LIN